26.12.2013 Views

Coherent Backscattering from Multiple Scattering Systems - KOPS ...

Coherent Backscattering from Multiple Scattering Systems - KOPS ...

Coherent Backscattering from Multiple Scattering Systems - KOPS ...

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

5.1 Conservation of energy in coherent backscattering<br />

1<br />

kl* = 2<br />

kl* = 4<br />

kl* = 10<br />

0.8<br />

cooperon<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

−90 −60 −30 0 30 60 90<br />

scattering angle [deg]<br />

Figure 5.5: Old and new theory. The graph shows the cooperon calculated with<br />

eqn. 2.15 (dashed lines) and including the additional contribution given in eqn. 5.7<br />

(solid lines). The dotted lines give the enhancement of the cooperon for the new theory<br />

(for the old theory the enhancement is always equal to 1). Parameters: wavelength<br />

λ = 590 nm, diffusion coefficient D = 15 m2 /s, reflectivity R = 0.5.<br />

The fit parameter a is therefore obtained by numerical integration of<br />

a =<br />

0<br />

∫ π/2<br />

0<br />

∫ π/2<br />

I (A)<br />

c<br />

1<br />

(kl ∗ ) 2 ·<br />

· sin θ dθ<br />

µ · sin θ dθ<br />

µ + 1<br />

After normalization analogous to eqns. 2.13, the additional contribution to the cooperon finally<br />

becomes<br />

α (B+C)<br />

c<br />

8π · a<br />

= −<br />

3 k 2 l ∗ (l ∗ + 2z 0 ) ·<br />

µ<br />

µ + 1<br />

(5.7)<br />

does not contribute at a specific angular value but it is rather spread out over the<br />

whole angular range, similar to the diffuson. In particular it reduces the enhancement of the<br />

coherent backscattering cone, so that the total cooperon α (A)<br />

c<br />

α (B+C)<br />

c<br />

+ α (B+C)<br />

c at the conetip at θ = 0<br />

51

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!